A Study of Transonic Flow and Airfoils. Presented by: Huiliang Lui 30 th April 2007
|
|
- Shannon Hunt
- 5 years ago
- Views:
Transcription
1 A Study of Transonic Flow and Airfoils Presented by: Huiliang Lui 3 th April 7
2 Contents Background Aims Theory Conservation Laws Irrotational Flow Self-Similarity Characteristics Numerical Modeling Conclusion
3 Background Transonic regime Loosely defined region of flow around sonic speed (free stream velocities.8 M 1. ) Mixed regions of locally subsonic and supersonic flow. Unpredictable effect of shockwaves on the control surfaces
4 Aims Expand knowledge of aerodynamics and compressible flow Investigate the effects of transonic flow on airfoils Analyze behavior of pressure coefficient, C p
5 Theory: Conservation Equations Euler s Equations: Continuity ρ + tt ( ρv ) = Momentum DV ρ Dt = p Energy Dh ρ o Dt = ρ t
6 Theory: Irrotational Flow Vorticity V r Vorticity = for irrotational flow Define: velocity potential Φ such that Why? V r Φ Simplifies conservation equations into one governing equation [1]: Φ 1 a Φ a x x Φ Φ y xx Φ xy Φ + 1 a y Φ xφ a z Φ Φ yy xz Φ + 1 a Φ a y Φ z z Φ Φ yz zz =
7 Theory: Irrotational Flow Validity for transonic flow: Entropy across shock [1] s γ 1 3 ( M ) 1 1 R s 3( γ + 1) For transonic, M 1 1 Flow can be assumed as isentropic, and therefore irrotational!
8 Theory: Irrotational Flow Introduce perturbation velocity potential: Φ = V x + φ Governing equation simplifies to: (1 = M M ) φ xx + φ Note: RHS drops out for subsonic or supersonic flow, resulting in linearized PDE. yy φx ( γ + 1) V + φ φ xx zz
9 Theory: Self-Similarity Recall governing equation: (1 M φ φ φ ) xx + yy + zz = M ( + 1) γ φx V φ xx Introduce slenderness ratio τ = b / c
10 Theory: Self-Similarity Self-similar variables: x = x c Nondimensionalize: y = φ = yτ c cv φ 1 3 Transonic similarity equation: where K = transonic similarity parameter: τ 3 z = zτ c [ K ( γ + 1) φ ] φ + φ + φ = K x xx 1 M = 3 τ yy zz 1 3
11 Theory: Characteristics Recall governing equation (D): 1 1 = Φ Φ Φ Φ Φ + Φ Φ xy y x yy y xx x a a a From midterm: 1 1 = + + a v dx dy a uv dx dy a u
12 Theory: Characteristics Solving, dy dx = uv ± a u + v ( a u ) a subsonic sonic supersonic elliptic parabolic hyperbolic Characteristic Slopes? Interpretation: The Mach Cone
13 Theory: Characteristics From NASAexplore s website:
14 Numerical Modeling Pressure coefficient po p CP = 1 ρv National Advisory Committee for Aeronautics (NACA) Data for foils Panel Methods
15 Panel Methods Basic principle: Superposition Boundary element method: Panels Sources/Sinks (simple solution) Vortices The Kutta Condition: Pressure above and below trailing edge must be equal
16 Strategy Attempt Vortex Panel method for three symmetric airfoils for linearized full potential equation (FPE) Help: ME163 website Extend to transonic modeling
17 Results: Symmetric Airfoils 8 NACA-1 Foil 8 NACA-15 Foil 6 6 y-c coordinate in % Airfoil Chord y-coordinate in % Airfoil Chord % Airfoil Chord % Airfoil Chord 1 NACA-18 Foil 8 y-coordinate in % Airfoil Chord % Airfoil Chord
18 Results: Linearized FPE 1.5 lower part upper part 1.5 lower part upper part C p -1 C p x-position x-position 1.5 lower part upper part -.5 C p x-position
19 Transonic Modeling Numerical solution is exponentially harder to obtain because of nonlinearity Make use of characteristics Further steps needed: Grid Generation: Solve FPE at nodes Discretization of the PDE Iterative solution
20 Sample Grid for NACA-1 1 x field panels (from GA Tech)
21 Results 1. Mach Number =.8 1. Mach Number = Mach Number = C p.6.4. C p.6.4. C p Mach Number = Mach Number = C p C p
22 Future Work Generate one case for nonlinear, transonic flow, and solve iteratively Validate with results from Oskam s article [5]: Transonic Panel Method for the Full Potential Equation Applied to Multicomponent Airfoils
23 Conclusion Better understanding of aerodynamics Application of mathematical methods for modeling Numerical modeling for nonlinear PDEs is significantly tougher than linearized PDEs Simplify PDEs whenever possible!
24 References 1.Anderson, J.D. Modern Compressible Flow. Houghton E.L. and Carpenter, P.W. Aerodynamics for Engineering Students 3. Ferrari, C. and Tricomi F.G. Transonic Aerodynamics 4. AE 393/493 Airfoil Design 5. Oskam, B. Transonic Panel Method for the Full Potential Equation Applied to Multicomponent Airfoils 6. ME163 Fall 6 Project Vortex Panel Method
Thin airfoil theory. Chapter Compressible potential flow The full potential equation
hapter 4 Thin airfoil theory 4. ompressible potential flow 4.. The full potential equation In compressible flow, both the lift and drag of a thin airfoil can be determined to a reasonable level of accuracy
More informationAA214B: NUMERICAL METHODS FOR COMPRESSIBLE FLOWS
AA214B: NUMERICAL METHODS FOR COMPRESSIBLE FLOWS 1 / 29 AA214B: NUMERICAL METHODS FOR COMPRESSIBLE FLOWS Hierarchy of Mathematical Models 1 / 29 AA214B: NUMERICAL METHODS FOR COMPRESSIBLE FLOWS 2 / 29
More informationDefinitions. Temperature: Property of the atmosphere (τ). Function of altitude. Pressure: Property of the atmosphere (p). Function of altitude.
Definitions Chapter 3 Standard atmosphere: A model of the atmosphere based on the aerostatic equation, the perfect gas law, an assumed temperature distribution, and standard sea level conditions. Temperature:
More informationSupersonic Aerodynamics. Methods and Applications
Supersonic Aerodynamics Methods and Applications Outline Introduction to Supersonic Flow Governing Equations Numerical Methods Aerodynamic Design Applications Introduction to Supersonic Flow What does
More informationNumerical Solution of Partial Differential Equations governing compressible flows
Numerical Solution of Partial Differential Equations governing compressible flows Praveen. C praveen@math.tifrbng.res.in Tata Institute of Fundamental Research Center for Applicable Mathematics Bangalore
More informationBasic Aspects of Discretization
Basic Aspects of Discretization Solution Methods Singularity Methods Panel method and VLM Simple, very powerful, can be used on PC Nonlinear flow effects were excluded Direct numerical Methods (Field Methods)
More informationCompressible Potential Flow: The Full Potential Equation. Copyright 2009 Narayanan Komerath
Compressible Potential Flow: The Full Potential Equation 1 Introduction Recall that for incompressible flow conditions, velocity is not large enough to cause density changes, so density is known. Thus
More informationAerodynamics. Lecture 1: Introduction - Equations of Motion G. Dimitriadis
Aerodynamics Lecture 1: Introduction - Equations of Motion G. Dimitriadis Definition Aerodynamics is the science that analyses the flow of air around solid bodies The basis of aerodynamics is fluid dynamics
More informationCHAPTER 7 SEVERAL FORMS OF THE EQUATIONS OF MOTION
CHAPTER 7 SEVERAL FORMS OF THE EQUATIONS OF MOTION 7.1 THE NAVIER-STOKES EQUATIONS Under the assumption of a Newtonian stress-rate-of-strain constitutive equation and a linear, thermally conductive medium,
More informationTo subsonic flow around the wing profile with shock waves in supersonic zones. Equation for stream function.
Global Journal of Pure and Applied Mathematics. ISSN 0973-1768 Volume 1, Number 4 (016), pp. 347-351 Research India Publications http://www.ripublication.com/gjpam.htm To subsonic flow around the wing
More informationPEMP ACD2505. M.S. Ramaiah School of Advanced Studies, Bengaluru
Governing Equations of Fluid Flow Session delivered by: M. Sivapragasam 1 Session Objectives -- At the end of this session the delegate would have understood The principle of conservation laws Different
More informationAOE 3114 Compressible Aerodynamics
AOE 114 Compressible Aerodynamics Primary Learning Objectives The student will be able to: 1. Identify common situations in which compressibility becomes important in internal and external aerodynamics
More information2. Getting Ready for Computational Aerodynamics: Fluid Mechanics Foundations
. Getting Ready for Computational Aerodynamics: Fluid Mechanics Foundations We need to review the governing equations of fluid mechanics before examining the methods of computational aerodynamics in detail.
More informationContinuity Equation for Compressible Flow
Continuity Equation for Compressible Flow Velocity potential irrotational steady compressible Momentum (Euler) Equation for Compressible Flow Euler's equation isentropic velocity potential equation for
More informationIntroduction to Aerospace Engineering
Introduction to Aerospace Engineering Lecture slides Challenge the future 3-0-0 Introduction to Aerospace Engineering Aerodynamics 5 & 6 Prof. H. Bijl ir. N. Timmer Delft University of Technology 5. Compressibility
More information1. (20 pts total 2pts each) - Circle the most correct answer for the following questions.
ME 50 Gas Dynamics Spring 009 Final Exam NME:. (0 pts total pts each) - Circle the most correct answer for the following questions. i. normal shock propagated into still air travels with a speed (a) equal
More information1. Introduction Some Basic Concepts
1. Introduction Some Basic Concepts 1.What is a fluid? A substance that will go on deforming in the presence of a deforming force, however small 2. What Properties Do Fluids Have? Density ( ) Pressure
More informationShock Reflection-Diffraction, Nonlinear Partial Differential Equations of Mixed Type, and Free Boundary Problems
Chapter One Shock Reflection-Diffraction, Nonlinear Partial Differential Equations of Mixed Type, and Free Boundary Problems Shock waves are steep fronts that propagate in compressible fluids when convection
More informationChapter 9 Flow over Immersed Bodies
57:00 Mechanics of Fluids and Transport Processes Chapter 9 Professor Fred Stern Fall 009 1 Chapter 9 Flow over Immersed Bodies Fluid flows are broadly categorized: 1. Internal flows such as ducts/pipes,
More informationSeveral forms of the equations of motion
Chapter 6 Several forms of the equations of motion 6.1 The Navier-Stokes equations Under the assumption of a Newtonian stress-rate-of-strain constitutive equation and a linear, thermally conductive medium,
More informationEdwin van der Weide and Magnus Svärd. I. Background information for the SBP-SAT scheme
Edwin van der Weide and Magnus Svärd I. Background information for the SBP-SAT scheme As is well-known, stability of a numerical scheme is a key property for a robust and accurate numerical solution. Proving
More informationDEVELOPMENT OF A THREE-DIMENSIONAL TIGHTLY COUPLED EULER/POTENTIAL FLOW SOLVER FOR TRANSONIC FLOW
DEVELOPMENT OF A THREE-DIMENSIONAL TIGHTLY COUPLED EULER/POTENTIAL FLOW SOLVER FOR TRANSONIC FLOW Yeongmin Jo*, Se Hwan Park*, Duck-Joo Lee*, and Seongim Choi *Korea Advanced Institute of Science and Technology,
More informationIntroduction and Basic Concepts
Topic 1 Introduction and Basic Concepts 1 Flow Past a Circular Cylinder Re = 10,000 and Mach approximately zero Mach = 0.45 Mach = 0.64 Pictures are from An Album of Fluid Motion by Van Dyke Flow Past
More informationCopyright 2007 N. Komerath. Other rights may be specified with individual items. All rights reserved.
Low Speed Aerodynamics Notes 5: Potential ti Flow Method Objective: Get a method to describe flow velocity fields and relate them to surface shapes consistently. Strategy: Describe the flow field as the
More informationGoverning Equations of Fluid Dynamics
Chapter 3 Governing Equations of Fluid Dynamics The starting point of any numerical simulation are the governing equations of the physics of the problem to be solved. In this chapter, we first present
More informationIn this section, mathematical description of the motion of fluid elements moving in a flow field is
Jun. 05, 015 Chapter 6. Differential Analysis of Fluid Flow 6.1 Fluid Element Kinematics In this section, mathematical description of the motion of fluid elements moving in a flow field is given. A small
More informationfor what specific application did Henri Pitot develop the Pitot tube? what was the name of NACA s (now NASA) first research laboratory?
1. 5% short answers for what specific application did Henri Pitot develop the Pitot tube? what was the name of NACA s (now NASA) first research laboratory? in what country (per Anderson) was the first
More informationTo study the motion of a perfect gas, the conservation equations of continuity
Chapter 1 Ideal Gas Flow The Navier-Stokes equations To study the motion of a perfect gas, the conservation equations of continuity ρ + (ρ v = 0, (1.1 momentum ρ D v Dt = p+ τ +ρ f m, (1.2 and energy ρ
More informationHigh Speed Aerodynamics. Copyright 2009 Narayanan Komerath
Welcome to High Speed Aerodynamics 1 Lift, drag and pitching moment? Linearized Potential Flow Transformations Compressible Boundary Layer WHAT IS HIGH SPEED AERODYNAMICS? Airfoil section? Thin airfoil
More informationAE/ME 339. Computational Fluid Dynamics (CFD) K. M. Isaac. Momentum equation. Computational Fluid Dynamics (AE/ME 339) MAEEM Dept.
AE/ME 339 Computational Fluid Dynamics (CFD) 9//005 Topic7_NS_ F0 1 Momentum equation 9//005 Topic7_NS_ F0 1 Consider the moving fluid element model shown in Figure.b Basis is Newton s nd Law which says
More informationFundamentals of Aerodynamics
Fundamentals of Aerodynamics Fourth Edition John D. Anderson, Jr. Curator of Aerodynamics National Air and Space Museum Smithsonian Institution and Professor Emeritus University of Maryland Me Graw Hill
More informationInvestigation potential flow about swept back wing using panel method
INTERNATIONAL JOURNAL OF ENERGY AND ENVIRONMENT Volume 7, Issue 4, 2016 pp.317-326 Journal homepage: www.ijee.ieefoundation.org Investigation potential flow about swept back wing using panel method Wakkas
More informationFundamentals of Aerodynamits
Fundamentals of Aerodynamits Fifth Edition in SI Units John D. Anderson, Jr. Curator of Aerodynamics National Air and Space Museum Smithsonian Institution and Professor Emeritus University of Maryland
More informationIntroduction to Aerodynamics. Dr. Guven Aerospace Engineer (P.hD)
Introduction to Aerodynamics Dr. Guven Aerospace Engineer (P.hD) Aerodynamic Forces All aerodynamic forces are generated wither through pressure distribution or a shear stress distribution on a body. The
More informationAE301 Aerodynamics I UNIT B: Theory of Aerodynamics
AE301 Aerodynamics I UNIT B: Theory of Aerodynamics ROAD MAP... B-1: Mathematics for Aerodynamics B-: Flow Field Representations B-3: Potential Flow Analysis B-4: Applications of Potential Flow Analysis
More informationViscous flow along a wall
Chapter 8 Viscous flow along a wall 8. The no-slip condition All liquids and gases are viscous and, as a consequence, a fluid near a solid boundary sticks to the boundary. The tendency for a liquid or
More information8. Introduction to Computational Fluid Dynamics
8. Introduction to Computational Fluid Dynamics We have been using the idea of distributions of singularities on surfaces to study the aerodynamics of airfoils and wings. This approach was very powerful,
More informationTwo Posts to Fill On School Board
Y Y 9 86 4 4 qz 86 x : ( ) z 7 854 Y x 4 z z x x 4 87 88 Y 5 x q x 8 Y 8 x x : 6 ; : 5 x ; 4 ( z ; ( ) ) x ; z 94 ; x 3 3 3 5 94 ; ; ; ; 3 x : 5 89 q ; ; x ; x ; ; x : ; ; ; ; ; ; 87 47% : () : / : 83
More informationMULTIGRID CALCULATIONS FOB. CASCADES. Antony Jameson and Feng Liu Princeton University, Princeton, NJ 08544
MULTIGRID CALCULATIONS FOB. CASCADES Antony Jameson and Feng Liu Princeton University, Princeton, NJ 0544 1. Introduction Development of numerical methods for internal flows such as the flow in gas turbines
More informationSimple waves and a characteristic decomposition of the two dimensional compressible Euler equations
Simple waves and a characteristic decomposition of the two dimensional compressible Euler equations Jiequan Li 1 Department of Mathematics, Capital Normal University, Beijing, 100037 Tong Zhang Institute
More informationCompressible Duct Flow with Friction
Compressible Duct Flow with Friction We treat only the effect of friction, neglecting area change and heat transfer. The basic assumptions are 1. Steady one-dimensional adiabatic flow 2. Perfect gas with
More informationAerothermodynamics of High Speed Flows
Aerothermodynamics of High Speed Flows Lecture 1: Introduction G. Dimitriadis 1 The sound barrier Supersonic aerodynamics and aircraft design go hand in hand Aspects of supersonic flow theory were developed
More informationIntroduction to Fluid Mechanics. Chapter 13 Compressible Flow. Fox, Pritchard, & McDonald
Introduction to Fluid Mechanics Chapter 13 Compressible Flow Main Topics Basic Equations for One-Dimensional Compressible Flow Isentropic Flow of an Ideal Gas Area Variation Flow in a Constant Area Duct
More informationM E 320 Professor John M. Cimbala Lecture 10
M E 320 Professor John M. Cimbala Lecture 10 Today, we will: Finish our example problem rates of motion and deformation of fluid particles Discuss the Reynolds Transport Theorem (RTT) Show how the RTT
More informationIntroduction to Fluid Mechanics
Introduction to Fluid Mechanics Tien-Tsan Shieh April 16, 2009 What is a Fluid? The key distinction between a fluid and a solid lies in the mode of resistance to change of shape. The fluid, unlike the
More informationLifting Airfoils in Incompressible Irrotational Flow. AA210b Lecture 3 January 13, AA210b - Fundamentals of Compressible Flow II 1
Lifting Airfoils in Incompressible Irrotational Flow AA21b Lecture 3 January 13, 28 AA21b - Fundamentals of Compressible Flow II 1 Governing Equations For an incompressible fluid, the continuity equation
More informationChapter 9: Differential Analysis
9-1 Introduction 9-2 Conservation of Mass 9-3 The Stream Function 9-4 Conservation of Linear Momentum 9-5 Navier Stokes Equation 9-6 Differential Analysis Problems Recall 9-1 Introduction (1) Chap 5: Control
More informationDrag of a thin wing and optimal shape to minimize it
Drag of a thin wing and optimal shape to minimize it Alejandro Pozo December 21 st, 211 Outline 1 Statement of the problem 2 Inviscid compressible flows 3 Drag for supersonic case 4 Example of optimal
More informationDirect Numerical Solution of the Steady 1D Compressible Euler Equations for Transonic Flow Profiles with Shocks
Direct Numerical Solution of the Steady 1D Compressible Euler Equations for Transonic Flow Profiles with Shocks Hans De Sterck, Scott Rostrup Department of Applied Mathematics, University of Waterloo,
More informationAE 2020: Low Speed Aerodynamics. I. Introductory Remarks Read chapter 1 of Fundamentals of Aerodynamics by John D. Anderson
AE 2020: Low Speed Aerodynamics I. Introductory Remarks Read chapter 1 of Fundamentals of Aerodynamics by John D. Anderson Text Book Anderson, Fundamentals of Aerodynamics, 4th Edition, McGraw-Hill, Inc.
More informationLength Learning Objectives Learning Objectives Assessment
Universidade Federal Fluminense PGMEC Course: Advanced Computational Fluid Dynamics Coordinator: Vassilis Theofilis Academic Year: 2018, 2 nd Semester Length: 60hrs (48hrs classroom and 12hrs tutorials)
More informationChapter 9: Differential Analysis of Fluid Flow
of Fluid Flow Objectives 1. Understand how the differential equations of mass and momentum conservation are derived. 2. Calculate the stream function and pressure field, and plot streamlines for a known
More information1. Fluid Dynamics Around Airfoils
1. Fluid Dynamics Around Airfoils Two-dimensional flow around a streamlined shape Foces on an airfoil Distribution of pressue coefficient over an airfoil The variation of the lift coefficient with the
More informationChapter 6: Incompressible Inviscid Flow
Chapter 6: Incompressible Inviscid Flow 6-1 Introduction 6-2 Nondimensionalization of the NSE 6-3 Creeping Flow 6-4 Inviscid Regions of Flow 6-5 Irrotational Flow Approximation 6-6 Elementary Planar Irrotational
More informationEfficient solution of stationary Euler flows with critical points and shocks
Efficient solution of stationary Euler flows with critical points and shocks Hans De Sterck Department of Applied Mathematics University of Waterloo 1. Introduction consider stationary solutions of hyperbolic
More informationRocket Thermodynamics
Rocket Thermodynamics PROFESSOR CHRIS CHATWIN LECTURE FOR SATELLITE AND SPACE SYSTEMS MSC UNIVERSITY OF SUSSEX SCHOOL OF ENGINEERING & INFORMATICS 25 TH APRIL 2017 Thermodynamics of Chemical Rockets ΣForce
More informationAerodynamics. High-Lift Devices
High-Lift Devices Devices to increase the lift coefficient by geometry changes (camber and/or chord) and/or boundary-layer control (avoid flow separation - Flaps, trailing edge devices - Slats, leading
More informationIterative Solution of Transonic Flows over Airfoils and Wings, Including Flows at Mach 1,
Iterative Solution of Transonic Flows over Airfoils and Wings, Including Flows at Mach 1, ANTONY JAMESON 1 Introduction Transonic aerodynamics is the focus of strong interest at the present time because
More informationFurther Studies of Airfoils Supporting Non-unique Solutions in Transonic Flow
29th AIAA Applied Aerodynamics Conference 27-30 June 2011, Honolulu, Hawaii AIAA 2011-3509 Further Studies of Airfoils Supporting Non-unique Solutions in Transonic Flow Antony Jameson, John C. Vassberg,
More informationACD2503 Aircraft Aerodynamics
ACD2503 Aircraft Aerodynamics Session delivered by: Prof. M. D. Deshpande 1 Aims and Summary PEMP It is intended dto prepare students for participation i i in the design process of an aircraft and its
More informationSHAPE OPTIMIZATION IN SUPERSONIC FLOW GRADUATION PROJECT. Mustafa Suphi Deniz KARANFIL. Department of Aeronautical Engineering
ISTANBUL TECHNICAL UNIVERSITY FACULTY OF AERONAUTICS AND ASTRONAUTICS SHAPE OPTIMIZATION IN SUPERSONIC FLOW GRADUATION PROJECT Mustafa Suphi Deniz KARANFIL Department of Aeronautical Engineering Thesis
More informationReview of Fundamentals - Fluid Mechanics
Review of Fundamentals - Fluid Mechanics Introduction Properties of Compressible Fluid Flow Basics of One-Dimensional Gas Dynamics Nozzle Operating Characteristics Characteristics of Shock Wave A gas turbine
More informationWings and Bodies in Compressible Flows
Wings and Bodies in Compressible Flows Prandtl-Glauert-Goethert Transformation Potential equation: 1 If we choose and Laplace eqn. The transformation has stretched the x co-ordinate by 2 Values of at corresponding
More informationChapter 4: Fluid Kinematics
Overview Fluid kinematics deals with the motion of fluids without considering the forces and moments which create the motion. Items discussed in this Chapter. Material derivative and its relationship to
More informationPartial Differential Equations
Partial Differential Equations Xu Chen Assistant Professor United Technologies Engineering Build, Rm. 382 Department of Mechanical Engineering University of Connecticut xchen@engr.uconn.edu Contents 1
More informationV (r,t) = i ˆ u( x, y,z,t) + ˆ j v( x, y,z,t) + k ˆ w( x, y, z,t)
IV. DIFFERENTIAL RELATIONS FOR A FLUID PARTICLE This chapter presents the development and application of the basic differential equations of fluid motion. Simplifications in the general equations and common
More informationIncompressible Flow Over Airfoils
Chapter 7 Incompressible Flow Over Airfoils Aerodynamics of wings: -D sectional characteristics of the airfoil; Finite wing characteristics (How to relate -D characteristics to 3-D characteristics) How
More informationChapter 9 Flow over Immersed Bodies
57:00 Mechanics of Fluids and Transport Processes Chapter 9 Professor Fred Stern Fall 014 1 Chapter 9 Flow over Immersed Bodies Fluid flows are broadly categorized: 1. Internal flows such as ducts/pipes,
More informationAeroelasticity. Lecture 9: Supersonic Aeroelasticity. G. Dimitriadis. AERO0032-1, Aeroelasticity and Experimental Aerodynamics, Lecture 9
Aeroelasticity Lecture 9: Supersonic Aeroelasticity G. Dimitriadis AERO0032-1, Aeroelasticity and Experimental Aerodynamics, Lecture 9 1 Introduction All the material presented up to now concerned incompressible
More informationMIRAMARE - TRIESTE June 2001
IC/2001/48 United Nations Educational Scientific and Cultural Organization and International Atomic Energy Agency THE ABDUS SALAM INTERNATIONAL CENTRE FOR THEORETICAL PHYSICS TRANSONIC AND SUPERSONIC OVERTAKING
More informationChapter 3 Second Order Linear Equations
Partial Differential Equations (Math 3303) A Ë@ Õæ Aë áöß @. X. @ 2015-2014 ú GA JË@ É Ë@ Chapter 3 Second Order Linear Equations Second-order partial differential equations for an known function u(x,
More informationPDE Solvers for Fluid Flow
PDE Solvers for Fluid Flow issues and algorithms for the Streaming Supercomputer Eran Guendelman February 5, 2002 Topics Equations for incompressible fluid flow 3 model PDEs: Hyperbolic, Elliptic, Parabolic
More informationTHE ELLIPTICITY PRINCIPLE FOR SELF-SIMILAR POTENTIAL FLOWS
Journal of Hyperbolic Differential Equations Vol., No. 4 005 909 917 c World Scientific Publishing Company THE ELLIPTICITY PRINCIPLE FOR SELF-SIMILAR POTENTIAL FLOWS VOLKER ELLING, and TAI-PING LIU, Dept.
More informationCapSel Euler The Euler equations. conservation laws for 1D dynamics of compressible gas. = 0 m t + (m v + p) x
CapSel Euler - 01 The Euler equations keppens@rijnh.nl conservation laws for 1D dynamics of compressible gas ρ t + (ρ v) x = 0 m t + (m v + p) x = 0 e t + (e v + p v) x = 0 vector of conserved quantities
More informationAPPLICATION OF SPACE-TIME MAPPING ANALYSIS METHOD TO UNSTEADY NONLINEAR GUST-AIRFOIL INTERACTION PROBLEM
AIAA 2003-3693 APPLICATION OF SPACE-TIME MAPPING ANALYSIS METHOD TO UNSTEADY NONLINEAR GUST-AIRFOIL INTERACTION PROBLEM Vladimir V. Golubev* and Axel Rohde Embry-Riddle Aeronautical University Daytona
More information4 Compressible Fluid Dynamics
4 Compressible Fluid Dynamics 4. Compressible flow definitions Compressible flow describes the behaviour of fluids that experience significant variations in density under the application of external pressures.
More informationA HARMONIC BALANCE APPROACH FOR MODELING THREE-DIMENSIONAL NONLINEAR UNSTEADY AERODYNAMICS AND AEROELASTICITY
' - ' Proceedings of ASME International Mechanical Engineering Conference and Exposition November 17-22, 22, New Orleans, Louisiana, USA IMECE-22-3232 A HARMONIC ALANCE APPROACH FOR MODELING THREE-DIMENSIONAL
More informationNonlinear system of mixed type and its application to steady Euler-Poisson system
The 1st Meeting of Young Researchers in PDEs Nonlinear system of mixed type and its application to steady Euler-Poisson system Myoungjean Bae (POSTECH) -based on collaborations with- B. Duan, J. Xiao,
More informationSummer AS5150# MTech Project (summer) **
AE1 - M.Tech Aerospace Engineering Sem. Course No Course Name Lecture Tutorial Extended Tutorial Afternoon Lab Session Time to be spent outside of class 1 AS5010 Aerodynamics and Aircraft 3 0 0 0 6 9 performance
More informationMANY BILLS OF CONCERN TO PUBLIC
- 6 8 9-6 8 9 6 9 XXX 4 > -? - 8 9 x 4 z ) - -! x - x - - X - - - - - x 00 - - - - - x z - - - x x - x - - - - - ) x - - - - - - 0 > - 000-90 - - 4 0 x 00 - -? z 8 & x - - 8? > 9 - - - - 64 49 9 x - -
More informationOWELL WEEKLY JOURNAL
Y \»< - } Y Y Y & #»»» q ] q»»»>) & - - - } ) x ( - { Y» & ( x - (» & )< - Y X - & Q Q» 3 - x Q Y 6 \Y > Y Y X 3 3-9 33 x - - / - -»- --
More informationIX. COMPRESSIBLE FLOW. ρ = P
IX. COMPRESSIBLE FLOW Compressible flow is the study of fluids flowing at speeds comparable to the local speed of sound. This occurs when fluid speeds are about 30% or more of the local acoustic velocity.
More informationManipulator Dynamics 2. Instructor: Jacob Rosen Advanced Robotic - MAE 263D - Department of Mechanical & Aerospace Engineering - UCLA
Manipulator Dynamics 2 Forward Dynamics Problem Given: Joint torques and links geometry, mass, inertia, friction Compute: Angular acceleration of the links (solve differential equations) Solution Dynamic
More informationFUNDAMENTALS OF AERODYNAMICS
*A \ FUNDAMENTALS OF AERODYNAMICS Second Edition John D. Anderson, Jr. Professor of Aerospace Engineering University of Maryland H ' McGraw-Hill, Inc. New York St. Louis San Francisco Auckland Bogota Caracas
More informationA DARK GREY P O N T, with a Switch Tail, and a small Star on the Forehead. Any
Y Y Y X X «/ YY Y Y ««Y x ) & \ & & } # Y \#$& / Y Y X» \\ / X X X x & Y Y X «q «z \x» = q Y # % \ & [ & Z \ & { + % ) / / «q zy» / & / / / & x x X / % % ) Y x X Y $ Z % Y Y x x } / % «] «] # z» & Y X»
More information0.2. CONSERVATION LAW FOR FLUID 9
0.2. CONSERVATION LAW FOR FLUID 9 Consider x-component of Eq. (26), we have D(ρu) + ρu( v) dv t = ρg x dv t S pi ds, (27) where ρg x is the x-component of the bodily force, and the surface integral is
More informationAerothermodynamics of high speed flows
Aerothermodynamics of high speed flows AERO 0033 1 Lecture 6: D potential flow, method of characteristics Thierry Magin, Greg Dimitriadis, and Johan Boutet Thierry.Magin@vki.ac.be Aeronautics and Aerospace
More informationTransonic Aerodynamics Wind Tunnel Testing Considerations. W.H. Mason Configuration Aerodynamics Class
Transonic Aerodynamics Wind Tunnel Testing Considerations W.H. Mason Configuration Aerodynamics Class Transonic Aerodynamics History Pre WWII propeller tip speeds limited airplane speed Props did encounter
More informationConfiguration Aerodynamics
Configuration Aerodynamics William H. Mason Virginia Tech Blacksburg, VA The front cover of the brochure describing the French Exhibit at the Montreal Expo, 1967. January 2018 W.H. Mason CONTENTS i CONTENTS
More informationAnalyses of Diamond - Shaped and Circular Arc Airfoils in Supersonic Wind Tunnel Airflows
Analyses of Diamond - Shaped and Circular Arc Airfoils in Supersonic Wind Tunnel Airflows Modo U. P, Chukwuneke J. L, Omenyi Sam 1 Department of Mechanical Engineering, Nnamdi Azikiwe University, Awka,
More informationAirfoils and Wings. Eugene M. Cliff
Airfoils and Wings Eugene M. Cliff 1 Introduction The primary purpose of these notes is to supplement the text material related to aerodynamic forces. We are mainly interested in the forces on wings and
More informationChapter 5. The Differential Forms of the Fundamental Laws
Chapter 5 The Differential Forms of the Fundamental Laws 1 5.1 Introduction Two primary methods in deriving the differential forms of fundamental laws: Gauss s Theorem: Allows area integrals of the equations
More informationDirect Numerical Simulations of Plunging Airfoils
48th AIAA Aerospace Sciences Meeting Including the New Horizons Forum and Aerospace Exposition 4-7 January 010, Orlando, Florida AIAA 010-78 Direct Numerical Simulations of Plunging Airfoils Yves Allaneau
More informationModule3: Waves in Supersonic Flow Lecture14: Waves in Supersonic Flow (Contd.)
1 Module3: Waves in Supersonic Flow Lecture14: Waves in Supersonic Flow (Contd.) Mach Reflection: The appearance of subsonic regions in the flow complicates the problem. The complications are also encountered
More informationPropulsion Systems and Aerodynamics MODULE CODE LEVEL 6 CREDITS 20 Engineering and Mathematics Industrial Collaborative Engineering
TITLE Propulsion Systems and Aerodynamics MODULE CODE 55-6894 LEVEL 6 CREDITS 20 DEPARTMENT Engineering and Mathematics SUBJECT GROUP Industrial Collaborative Engineering MODULE LEADER Dr. Xinjun Cui DATE
More informationAerodynamics. Basic Aerodynamics. Continuity equation (mass conserved) Some thermodynamics. Energy equation (energy conserved)
Flow with no friction (inviscid) Aerodynamics Basic Aerodynamics Continuity equation (mass conserved) Flow with friction (viscous) Momentum equation (F = ma) 1. Euler s equation 2. Bernoulli s equation
More informationFinal: Solutions Math 118A, Fall 2013
Final: Solutions Math 118A, Fall 2013 1. [20 pts] For each of the following PDEs for u(x, y), give their order and say if they are nonlinear or linear. If they are linear, say if they are homogeneous or
More informationInfluence of Molecular Complexity on Nozzle Design for an Organic Vapor Wind Tunnel
ORC 2011 First International Seminar on ORC Power Systems, Delft, NL, 22-23 September 2011 Influence of Molecular Complexity on Nozzle Design for an Organic Vapor Wind Tunnel A. Guardone, Aerospace Eng.
More informationIntroduction to Aerospace Engineering
Introduction to Aerosace Engineering Lecture slides hallenge the future Introduction to Aerosace Engineering Aerodynamics & Prof. H. Bijl ir. N. Timmer &. Airfoils and finite wings Anderson 5.9 end of
More information